SL 2 ℝ × U 1 U 1 $$ \frac{\mathrm{SL}\left(2,\mathrm{\mathbb{R}}\right)\times \mathrm{U}(1)}{\mathrm{U}(1)} $$ CFT, NS5+F1 system and single trace T T ¯ $$ T\overline{T} $$

SL 2 ℝ × U 1 U 1 $$ \frac{\mathrm{SL}\left(2,\mathrm{\mathbb{R}}\right)\times \mathrm{U}(1)}{\mathrm{U}(1)} $$ CFT, NS5+F1 system and single trace T T ¯ $$ T\overline{T} $$

Abstract In this paper we prove the equivalence among (i) the weakly coupled worldsheet string theory described by the coset sigma model SL 2 ℝ k × U 1 U 1 $$ \frac{\mathrm{SL}{\left(2,\mathrm{\mathbb{R}}\right)}_k\times \mathrm{U}(1)}{\mathrm{U}(1)} $$ × S 3 × T 4 with SL(2, ℝ) WZW level k ≥ 2, (ii...

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Bibliographic Details
Main Author: Soumangsu Chakraborty
Format: Article
Language:English
Published: SpringerOpen 2021-03-01
Series:Journal of High Energy Physics
Subjects:
Gauge-gravity correspondence
Long strings
Sigma Models
Online Access:https://doi.org/10.1007/JHEP03(2021)113

Internet

https://doi.org/10.1007/JHEP03(2021)113

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